Phenomenology of an $SU(2)_1 \times SU(2)_2 \times U(1)_Y$ model at the LHC

Chuan-Hung Chen; Takaaki Nomura

doi:10.1103/PhysRevD.95.015015

paper

Phenomenology of an $S U (2)_{1} \times S U (2)_{2} \times U (1)_{Y}$ model at the LHC

arXiv:1606.03804 · doi:10.1103/PhysRevD.95.015015

Abstract

We investigate the implications of a minimal $S U (2)$ gauge symmetry extension of the standard model at the LHC. To achieve the spontaneous symmetry breaking, a heavy Higgs doublet of the $S U (2)$ is introduced. To obtain an anomaly free model and the decays of new charged gauge bosons, we include a vector-like quark doublet. We also employ a real scalar boson to dictate the heavy Higgs production via the gluon-gluon fusion processes. It is found that the new gauge coupling and the masses of new gauge bosons can be strictly bounded by the electroweak $ρ$ -parameter and dilepton resonance experiments at the LHC. It is found that due to the new charged gauge boson enhancement, the cross sections for a heavy scalar boson to diphoton channel measured by ATLAS and CMS can be easily satisfied when the values of Yukawa couplings are properly taken. Furthermore, by adopting event simulation, we find that the significance of $pp \to (γ γ)_{H} + jet$ , where the diphoton is from the heavy Higgs decay, can be over $4 σ$ when the luminosity is above 60 fb $^{- 1}$ .

22 pages, 5 figures, 3 tables, version accepted by Phys. Rev. D

Phenomenology of an $S U (2)_{1} \times S U (2)_{2} \times U (1)_{Y}$ model at the LHC

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Phenomenology of an SU(2)1​×SU(2)2​×U(1)Y​ model at the LHC

Abstract

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Phenomenology of an $S U (2)_{1} \times S U (2)_{2} \times U (1)_{Y}$ model at the LHC